METHOD FOR OBSERVING DYNAMIC PHYSICAL PROPERTY OF BIOLOGICAL TISSUE AND DEVICE FOR OBSERVING DYNAMIC PHYSICAL PROPERTY OF BIOLOGICAL TISSUE

Information

  • Patent Application
  • 20190128804
  • Publication Number
    20190128804
  • Date Filed
    April 20, 2017
    7 years ago
  • Date Published
    May 02, 2019
    5 years ago
Abstract
Biological tissues such as cartilage tissue and regenerated tissues such as regenerated cartilage are evaluated. Provided is a method for observing a dynamic physical property of a biological tissue by irradiating the biological tissue with a pulsed light having a wavelength of a far-infrared wavelength region to observe the dynamic physical property of the biological tissue using vibrational optical activity spectroscopy. When a sample which is the biological tissue is irradiated with a pulsed light, the biological tissue is vibrated. A relaxation time is obtained on the basis of a vibrational circular dichroism spectrum and/or a polarization spectroscopy spectrum which are/is obtained from a time-series signal of a reflected pulsed light reflected by the biological tissue or a transmitted pulsed light transmitted through the biological tissue.
Description
TECHNICAL FIELD

The present invention relates to a method for observing a dynamic physical property of a biological tissue and a device for observing a dynamic physical property of a biological tissue.


BACKGROUND ART

As society experiences aging of population, the number of patients suffering from diseases of organs of locomotion as represented by locomotive syndrome, in particular joint diseases has been increasing. One of the joint diseases is osteoarthritis, osteoarthritis is rarely healed spontaneously once a patient develops it, which generally progresses irreversibly and makes it difficult for him/her to walk. Therefore, osteoarthritis is one of the major factors lowering the quality of life of middle-aged and elderly people.


From the viewpoint of, for example, maintenance of the patient's quality of life, there has been increasing needs for early diagnosis and early treatment of osteoarthritis. In recent years, as an early treatment of osteoarthritis, treatment by regenerated cartilage transplantation is performed.


CITATION LIST
Patent Literature

[PTL 1] Japanese Unexamined Patent Application, Publication No. 2001-141567


SUMMARY OF INVENTION
Technical Problem

Regenerated tissue products such as regenerated cartilage involve a unique problem that they cannot be subjected to destruction inspection. As a result, in the current situations, regenerated tissues are transplanted without evaluation of their quality. Accordingly, development of a technique for noninvasively evaluating the regenerated tissues has been sought for.


Cartilage tissues are composed of chondrocytes and an extracellular matrix. In the extracellular matrix, macromolecules such as collagen, hyaluronic acid, sulfated glycosaminoglycan exist. The extracellular matrix constructs highly hydrated tissues by trapping a lot of water molecules and achieves high viscoelasticity of cartilage tissue and the like.


Regenerated cartilage uses chondrocytes collected and cultured from a living body and formed by a three-dimensional culture carrier, the chondrocytes, and the matrix produced by the chondrocytes.


Living tissues such as cartilage tissue and regenerated tissues such as regenerated cartilage are complex in structure and difficult to analyze. Patent Literature 1 discloses techniques for measuring an object to be measured such as a biopolymer which has been difficult to measure by conventional spectroscopic methods. However, in Patent Literature 1, it has not been possible to evaluate biological tissues such as cartilage tissue and regenerated tissues such as regenerated cartilage.


The present invention has been made in view of such circumstances, and it is an object of the present invention to provide a technique capable of evaluating biological tissues such as cartilage tissue and regenerated tissues such as regenerated cartilage.


Solution to Problem

The present invention provides a method for observing a dynamic physical property of a biological tissue by irradiating the biological tissue with a pulsed light having a wavelength of a far-infrared wavelength region to observe the dynamic physical property of the biological tissue using vibrational optical activity spectroscopy, where the biological tissue is vibrated while the biological tissue is being irradiated with the pulsed light.


A cartilage tissue is a tissue containing a lot of water, water molecules trapped in the extracellular matrix exist not as free water but as confined water in a state trapped and oriented in macromolecules such as the extracellular matrix.


The inventors of the present invention focused on the fact that the confinement of water molecules appears as a viscosity against the deformation due to compressive stress applied to the cartilage tissue, though that the degree of tissue formation and the dynamic physical property of the cartilage tissue could be estimated by measuring the state of the water molecules in the cartilage tissue, and conducted examinations and experimentations.


Vibration optical activity (abbreviated as VOA) spectroscopy is a scheme for measuring the difference in spectra for left and right circular polarized lights indicated by optically active molecules and examining steric information of molecules together with information on the vibration spectrum.


A terahertz wave resides in the far-inftared region and has good transmittivity to biological tissues. Since terahertz waves overlap with energy bands of intermolecular vibration and intramolecular vibration, it is possible to obtain information on tissue formation of biological tissues including cartilage tissue.


The terahertz wave has low photon energy and difficult to detect because it is hidden by noise in intensity or energy spectrum. As a result of intensive research, the inventors of the present invention have found that by using vibration optical activity spectroscopy in the terahertz band, it is made possible to obtain a spectrum attributable to the motion modes of water molecules (slow Debye relaxation mode, early Debye relaxation mode, intermolecular stretching vibration mode, and intermolecular declination vibration mode).


When the biological tissue is irradiated with a pulsed light, the biological tissue is vibrated. By forcibly imparting vibration to the biological tissue to cause the biological tissue to vibrate, it is made possible to perform spectroscopic measurement in accordance with the vibration frequency for imparting the vibration and gather an increased amount of information on the biological tissue at the molecule level. It is preferable to sweep the vibration frequency within a predetermined range.


For example, when a relaxation time of the biological tissue is to be obtained as the dynamic physical property, the vibration frequency dependence of the relaxation time can be revealed, which contributes to elucidation of the structure of the biological tissue.


In accordance with one aspect of the above-described invention, a radiation means is used, which has a photoconductive film receiving a pulse excitation light and generating a photocarrier and a pair of antenna electrode films formed on the photoconductive film and facing each other via a gap, wherein the radiation means is configured to emit the pulsed light having the wavelength of the fai-infrared wavelength region by pulsed laser light irradiation; the biological tissue is irradiated with the pulsed light from the radiation means while vibrating the biological tissue; and the dynamic physical property of the biological tissue is observed based on a vibrational circular dichroisn spectrum and/or polarization spectroscopy spectrum obtained from a time-series signal of a reflected pulsed light reflected by the biological tissue or a transmitted pulsed light transmitted through the biological tissue.


In addition, the present invention provides a device for observing a dynamic physical property of a biological tissue. The device includes a radiation means including a photoconductive film receiving an excitation pulsed laser light and generating a photocarrier and an antenna electrode film formed on the photoconductive film, and configured to emit a pulsed light having a wavelength of a far-infrared wavelength region by irradiation of the excitation pulsed laser light; a holding means configured to hold the biological tissue; a vibration device configured to vibrate the holding means; a detection means including a photoconductive film and an antenna electrode film and configured to obtain a time-series signal of a reflected pulsed light reflected by the biological tissue or a transmitted pulsed light transmitted through the biological tissue; and a control means configured to observe the dynamic physical property of the biological tissue based on a vibrational circular dichroism spectrum and/or polarization spectroscopy spectrum obtained from a signal obtained from the detection means.


Vibrations are forcibly imparted to the holding means holding the biological tissue with a vibration device. By virtue of this, it is made possible to perform spectroscopic measurement in accordance with the vibration frequency for imparting the vibrations and gather information on the biological tissue at the molecule level. It is preferable to sweep the vibration frequency within a predetermined range.


For example, when a relaxation time of the biological tissue is to be obtained as the dynamic physical property, the vibration frequency dependence of the relaxation time can be revealed, which contributes to the elucidation of the structure of the biological tissue.


As a device for imparting the vibrations, for example, piezoelectric elements such as PZT element may be used.


Preferably, it is preferable that the holding means includes a metamaterial. By virtue of this, the measurement sensitivity can be increased. The metamaterial is a substance in which minute units called “unit elements” are artificially arranged with equal intervals at distances sufficiently smaller than the wavelength of electromagnetic waves and the metamaterial is configured to behave as a homogeneous medium for electromagnetic waves.


Advantageous Effects of Invention

According to the present invention, it is made possible to provide a technique for observing the degree of tissue formation and dynamic physical property of biological tissues such as cartilage tissue and regenerated tissues such as regenerated cartilage based on vibrational optical activity obtained by using terahertz waves.


In addition, since the biological tissue is vibrated while being irradiated with the pulsed light, it is made possible to perform spectroscopic measurement in accordance with the vibration frequency for imparting the vibration and gather an increased amount of information on the biological tissue at the molecule level.





BRIEF DESCRIPTION OF DRAWINGS


FIG. 1 is a schematic diagram of a device for observing a dynamic physical property of a biological tissue according to one embodiment of the present invention.



FIG. 2 is a plan view of a pattern of an antenna electrode film.



FIG. 3 is a diagram illustrating a polarized pulsed light.



FIG. 4 is a configuration diagram in which an observation unit optical system is illustrated.



FIG. 5 is a longitudinal cross-sectional view illustrating a holding means.



FIG. 6 is a graph illustrating an example of measured data.



FIG. 7 is a graph obtained by data processing using two-dimensional correlation spectroscopy.





DESCRIPTION OF EMBODIMENTS


FIG. 1 illustrates an example of a device for observing a dynamic physical property of a biological tissue according to the present embodiment.


The device for observing the dynamic physical property of the biological tissue includes a pulsed laser light source 1. An ultrashort pulsed laser is used to configure the pulsed laser light source 1. The ultrashort pulsed laser may include a femtosecond fiber laser, a femtosecond mode-locked titanium sapphire laser, and the like.


The femtosecond fiber laser is configured, for example, by an LD-pumped passive mode-locked fiber laser using a 1.55 μm band erbium (Er) doped fiber laser as a laser gain medium. The femtosecond fiber laser may be an ytterbium (Yb) doped fiber with relatively wide band and high quantum effect around 1.06 μm.


The femtosecond fiber laser is used, for example, at a center oscillation wavelength (second harmonic output) of 780 nm, a pulse width of 120 to 75 fs (femtoseconds), an average output of 30 mW, and a cyclic frequency of around 40 MHz.


In the femtosecond mode-locked titanium sapphire laser, a titanium doped sapphire (Ti:Al2O3) crystal is used as the laser medium. Titanium doped sapphire crystal is superior for stable oscillation of femtosecond pulses.


The femtosecond mode-locked titanium sapphire laser is used, for example, at a central oscillation wavelength of 780 nm, a pulse width of 100 to 45 fs, an average output of 100 mW, and a cyclic frequency of about 40 to 80 MHz.


In comparison with femtosecond mode-locked titanium sapphire laser, the femtosecond fiber laser has superior advantages in practical use in terms of its small size, light weight, simple stable operation, low cost, and low power consumption. On the other hand, the femtosecond mode-locked titanium-sapphire laser has advantages such as relatively wide spectral bandwidth compared with that of the femtosecond fiber laser, excellent ultrashort pulsed light oscillation, and facilitated high-output oscillation.


The device for observing the dynamic physical property of the biological tissue further includes a beam splitter (splitting means) 2 configured to split the femtosecond laser light (pulsed laser light) L1 emitted from the pulsed laser light source 1 into pulsed laser light L2 for use in excitation and pulsed laser light L3 for use in detection.


The device for observing the dynamic physical property of the biological tissue further includes a terahertz wave generation element (radiation means) 3 configured to emit a pulsed light having a wavelength of a far-infrared wavelength region by irradiation of the pulsed laser light L2 for excitation and a detection element (detection means) 4 configured to detect a time-series signal of the electric field intensity of a transmitted pulsed light (or reflected pulsed light) from the biological tissue irradiated with the pulsed light from the terahertz wave generation element 3. Super-hemispherical silicon lenses 5, 6 are arranged on the light emission side of the terahertz wave generation element 3 and the light incident side of the detection element 4, respectively, as illustrated in FIG. 1.


The terahertz wave generation element 3 and the detection element 4 are photoconductive antenna (abbreviated as pca) elements. The PCA elements include a photoconductive film and an antenna electrode film.


The photoconductive film is formed, for example, by laminating a thin film of low temperature grown gallium arsenide (abbreviated as LT-GaAs) upon a semi-insulating gallium arsenide (abbreviated as SI-GaAs) substrate.


The antenna electrode film is laminated on the LT-GaAs photoconductive film. The material of the antenna electrode film may include gold (Au), etc. The antenna electrode film can be formed on the LT-GaAs thin layer by a vapor-deposition technique.



FIG. 2 is a plan view illustrating a pattern of the antenna electrode film according to the present embodiment. The antenna electrode film is configured by a pair of first antenna electrode films 7a arranged to face each other via a gap 8 and a pair of or multiple pairs of second antenna electrode films 7b arranged to face each other via the gap 8. The gap 8 is shared by the first antenna electrode films 7a and the second antenna electrode films 7b.


The pair of second antenna electrode films 7b is arranged with an angle with respect to the pair of first antenna electrode films 7a. In FIG. 2, the second antenna electrode films 7b in a plan view are arranged with an orientation different by substantially 90 degrees with respect to (substantially orthogonal to) the pair of first antenna electrode films 7a. Specifically, in the antenna electrode film, the pair of first antenna electrode films 7a and the pair of second antenna electrode films 7b have an orthogonal two-axis structure.


The first antenna electrode film 7a and the second antenna electrode film 7b are each configured by a conductive transmission channel 9 and a discharge electrode 10. The tip of the discharge electrode 10 is oriented toward the gap 8.


The pattern of the antenna electrode films can be adopted as appropriate depending on the frequency band of the terahertz wave to be emitted. For example, the outer-path interval d1 of the conductive transmission channel 9 is defined as 30 μm and the gaps d2 of the discharge electrodes 10 facing each other are both defined as 3 μm.


A first lead 11 is connected to the conductive transmission channel 9 of the first antenna electrode film 7a such that voltage can be applied to the pair of first antenna electrode films 7a. a second lead 12 is connected to the conductive transmission channel 9 of the second antenna electrode film 7b such that voltage can be applied to the pair of second antenna electrode films 7b. The other ends of the first lead and the second lead are connected to the modulation means 13 illustrated in FIG. 1.


The modulation means 13 has a voltage generation device (voltage generation unit) capable of applying bias voltage independently to both the first antenna electrode film 7a and the second antenna electrode film 7b. The modulation means 13 is capable of receiving signals from the control means 14 and modulating the phase, the amplitude, and the cyclic frequency.


A holding means 15 configured to hold a biological tissue (sample) is provided in an observation unit optical system 30 between the terahertz wave generation element 3 and the detection element 4. The term “biological tissue” may include biological tissues such as cartilage tissue and regenerated tissues such as regenerated cartilage.



FIG. 4 illustrates an example of the observation unit optical system 30. It should be noted that, while the optical axis in FIG. 4 extends in the longitudinal direction, which differs from the example illustrated in FIG. 1, the example of FIG. 4 can also be adopted with its optical axis extending in the width direction as illustrated in FIG. 1. The observation unit optical system 30 is of a Cassegrain type as illustrated in FIG. 4. A primary mirror 31 and a secondary mirror 32 are arranged at the side opposed to the holding means 15 (the upper portion in the same figure). The pulsed light incident from above in the figure is reflected by the secondary mirror 32 and then reflected by the primary mirror 31 and travels toward the holding means 15. The focal point resides at the location of the holding means 15, and the biological tissue handled as the sample is arranged at this location. The transmitted pulsed light that has transmitted through the biological tissue further transmits through the holding means 15 and travels downward, and is guided to the detection-side optical path. It should be noted that, when the reflected pulsed light that has been reflected by the biological tissue is to be used, the reflected pulsed light is reflected by the primary mirror 31 and the secondary mirror 32, then travels toward the incidence side (the upper portion in the figure) and guided to the detection-side optical path.



FIG. 5 illustrates a specific configuration of the holding means 15. As illustrated in this figure, the holding means 15 includes a supporting substrate 40, a metamaterial 41 arranged on the supporting substrate 40, and an insulating film 42 arranged on the metamaterial 41 such as silicon dioxide (SiO2), etc. Also, a piezoelectric element (vibration device) 43 such as a PZT element, etc. is provided on the side portion on the insulating film 42. In the same figure, the sample (biological tissue) S placed on the insulating film 42 is also illustrated. The sample S is cut into a thickness of several micrometers to several tens of micrometers, for example.


The metamaterial 41 is a substance in which minute units called “unit elements” are artificially arranged with equal intervals at distances sufficiently smaller than the wavelength of electromagnetic waves and the metamaterial 41 is configured to behave as a homogeneous medium for electromagnetic waves.


A not-shown power feeding cable and a not-shown control signal cable are connected to the piezoelectric element 43, and the piezoelectric element 43 is controlled by the control means 14. The piezoelectric element 43 is configured to be subjected to sweeping in accordance with a command from the control means 14, with a vibration frequency f [kHz] within a predetermined range, for example, from several kilohertz to several hundred hertz. The vibration frequency of the piezoelectric element 43 at the time of the measurement is captured in a storage area of the control means 14 along with the elapsed time. It should be noted that, while the piezoelectric elements 43 are provided on both sides of the insulating film 42 in FIG. 5, the number of the piezoelectric elements may be one or three or more as long as it is capable of imparting vibrations to the sample 3, and the locations of installation thereof are not limited to the side portion.


As illustrated in FIG. 1, an optical delay means 16 for time origin adjustment and an optical delay means 17 for time-series signal measurement are arranged on a detection-side optical path extending from the beam splitter 2 to the detection element 4. The order of arrangement of the optical delay means 16 for time origin adjustment and the optical delay means 17 for time-series signal measurement may be inverted.


The optical delay means 16, 17 each include two corner cube mirrors 18. The corner cube mirror 19 is fixed to an automatic feeding stage driven along a single axis and configured to change in a stepwise manner (or successively) the length of the light path from the beam splitter 2 to the detection element 4 by virtue of the stage feeding. The movement of the stage can be measured, by the He—Ne laser 19.


The optical delay means 16, 17 having the above-described configuration have the characteristic that the length of the light path can be changed two times as large as that in a case of one single corner cube mirror for scanning of the corner cube mirror. Accordingly, the effect achieved by these means is that it is made possible to specify settings for prompt time origin adjustment and the time-series signal measurement.


A driving device (trigger generation circuit) 20 that automatically carries out scanning is connected to the optical delay means 16 for time origin adjustment and the optical delay means 17 for time-series signal measurement, and the control means 14 that automatically controls the driving device 20 is also connected thereto.


An elliptical mirror (aspherical mirror) 21 and a plane mirror 22 are provided as optical elements on the incidence-side light path between the terahertz wave generation element 3 and the holding means 15. The elliptical mirror 21 is configured to concentrate the pulsed light from the terahertz wave generation element 3. The plane mirror 22 is arranged in the light path between the terahertz wave generation element 3 and the elliptical mirror 21 and has the redirection function for redirecting the pulsed light from the terahertz wave generation element 3. it should be noted that, while one elliptical mirror 21 and one plane mirror 22 are provided as in the case of the present embodiment, multiple elliptical mirrors 21 and multiple plane mirrors 22 can be used in combination.


An elliptical mirror (aspherical mirror) 23 and a plane mirror 24 are provided as optical elements on the detection-side optical path between the detection element 4 and the holding means 15. The elliptical mirror 23 is configured to concentrate the transmitted pulsed light from the sample. The plane mirror 24 is arranged on the light path between the elliptical mirror 23 and the detection element 4, and has the redirection function for redirecting the transmitted pulsed light from the elliptical mirror 23. It should be noted that, while one elliptical mirror 23 and one plane mirror 24 are provided as in the case of the present embodiment, multiple elliptical mirrors 23 and multiple plane mirrors 24 can be used in combination.


A current voltage conversion means (AVC) 25 is connected to the detection element 4. The AVC 25 is configured to convert the current signal that has been detected by the detection element 4 into a voltage signal.


A control means 14 is connected to the modulation means 13 and the current voltage conversion means 25 directly and via the lock-in amplifier 26. The control means 14 is capable of controlling the application of voltage to the antenna electrode films by the modulation means 13.


The control means 14 includes an analog-to-digital (A/D) converter 14a, an information processing unit 14b, and an input/output unit 14c. The information processing unit 14b is configured by, for example, a central processing unit (CPU), a random access memory (RAM), a read only memory (ROM), a computer readable storage medium, and the like. In addition, the series of processes for realizing the various functions are as an example stored in a storage medium or the like in the form of a program, and the various functions are realized by the CPU reading the program from the RAM or the like and carrying out information processing and arithmetic processing, it should be noted that various modes may be implemented for the program, such as a mode according to which the program is installed in advance in the ROM or another storage medium, a mode according to which the program is provided in a state where the program is stored in a computer-readable storage medium, and a mode according to which the program is distributed by wired or wireless communication means. The computer-readable storage medium refers to a magnetic disk, a magneto-optical disk, a CD-ROM disc, a dvd-eom disc, a semiconductor memory, and the like.


The control means 14 is configured to control the device for observing the dynamic physical property of the biological tissue and has the functions for computing and displaying data acquired by measurements.


Next, the operation of the device for observing the dynamic physical property of the biological tissue according to the present embodiment will be described.


The pulsed laser light L1 emitted from the pulsed laser light source 1 is split by the beam splitter 2 into the pulsed laser light (pump pulsed light) L2 for use in excitation and the pulsed laser light (sampling pulsed light) L3 for use in detection.


The excitation pulsed laser light L2 is emitted via the lens 27 to the terahertz wave generation element 3. At this point, the excitation pulsed laser light is concentrated onto the photoconductive film provided in the gap 8 of the antenna electrode film. In a state where bias voltage is applied to the antenna electrode film, when the photoconductive film is irradiated with the excitation pulsed laser light L2, the current due to the light excitation flows instantaneously, and a far-infrared electromagnetic pulse (pulsed light) is emitted.


At this point, the modulation means 13, in accordance with a command issued from the information processing unit 14b, simultaneously applies bias voltages to the first antenna electrode film 7a and the second antenna electrode film 7b, where the bias voltages have the same amplitude and period but the different phases shifted relative to each other, and modulates the pulsed light into a circular polarized light (see (a) and (b) of FIG. 3).


When not only the phase but the amplitude of the sinusoidal voltage applied to the second antenna electrode film 7b are differentiated, the pulsed light in the form of an elliptically polarized light will be emitted. By such a use, vibrational circular dichroism measurement can be performed.


The pulsed light, after its optical path is redirected by the plane mirror 22, is guided to the elliptical mirror 21 and concentrated so that the sample S is irradiated therewith. At this point, vibrations are forcibly imparted to the sample S by the piezoelectric element 43. The control means 14 carries out the sweeping with a vibration frequency f [kHz] within a predetermined range, in the presence of the metamaterial 41, the sample S is irradiated with the pulsed light and accordingly an increased amount of optical information will be transmitted or reflected.


The transmitted pulsed light that has transmitted the sample S and carries the optical information of the sample (or a reflected pulsed light that has been reflected by the sample) is reflected by the elliptical mirror 23 and then redirected by the plane mirror 24, and further guided to the detection element 4. At this point, the reflected or transmitted pulsed light is concentrated onto the photoconductive film residing in the gap 6 of the antenna electrode films.


The detection pulsed laser light L3 resulting from the splitting by the beam splitter 2 is given a delay time difference at predetermined time intervals by the optical delay means 16 for time origin adjustment and the optical delay means 17 for time-series signal measurement and guided to the detection element 4. At this point, the detection pulsed laser light L3 is concentrated onto the photoconductive film residing in the gap 8 of the antenna electrode films, and superposed on the reflected or transmitted pulsed light of the sample.


The detection element 4 will exhibit conductivity for the moment during which the photoconductive film is irradiated with the detection pulsed laser light L3. Hence, the electric field intensity and the phase lead of the reflected or transmitted pulsed light from the sample to which a trigger is applied and which has arrived at the moment at which the detection element 4 has become conductive are detected as the current signal.


The current signal that has been detected by the detection element 4 is converted into a voltage signal and amplified by the current voltage conversion means 25 and the voltage signal is sent to the lock-in amplifier 26. The pulsed light emitted from the terahertz wave generation element 3 is modulated by the modulation means 13, and the lock-in amplifier 26 uses the cyclic frequency of the modulated pulsed light as the reference signal, picks up only the voltages synchronized with the reference signal using a frequency filter, and the signal is detected with the influence of the background noise decreased.


The voltage signal that has been amplified by the lock-in amplifier 26 is converted into a digital signal by the A/D converter 14a. The information processing unit 14b performs Fourier transformation on the digital signal and calculates the amplitude of the electric field, intensity and the spectroscopic spectrum of the phase of the reflected or transmitted pulsed light of the sample.


The control means 14 obtains the polarization spectrum by standardizing spectroscopic spectra that have been obtained or obtaining the difference of them using the spectrum in a case where the sample does not exist. The control means 14 obtains the vibrational circular dichroism spectrum (VCD spectrum) by obtaining the difference of the left and right polarized lights of the spectroscopic spectra that have been obtained. The control means 14 can obtain the dynamic physical property of the sample based on the polarization spectrum and the vibrational circular dichroism spectrum that have been obtained, and observe them. The dynamic physical property may include elastic modulus (η), dielectric constant (ε), relaxation time (T1), refractive index.



FIG. 6 illustrates a vcd spectrum of an optical rotatory dispersion α*(σ) or a circular polarization dichroism ellipticity θ*(σ) which are examples of optically active amount or optical physical property amount acquired by the above-described device for observing the dynamic physical property of the biological tissue. Here, σ represents the wave number. In this figure, the horizontal axis represents time t, the vertical axis represents the optical rotatory dispersion α*(σ) or circular polarization dichroism ellipticity θ*(σ), and the depth axis represents the wave number σ[cm−1]. The graph illustrated in FIG. 6 can be computed by the control means 14 to be displayed.


As can be appreciated from the same figure, the waveform whose maximum and minimum are conspicuously distinct from each other at the beginning of the measurement is gradually attenuated with the passage of time. And the relaxation time T can be obtained from the attenuation of the wave numbers σ1 and σ2 representing the maximum value. For example, the relaxation time T of the optical rotatory dispersion α*(σ) can be obtained from the following expression:





α*(σ)=exp(t/T)


where t is the elapsed time.


Next, data processing using the two-dimensional correlation spectroscopy will be described. For the general understanding of the two-dimensional correlation spectroscopy, “Experimental Infrared Spectroscopy Fundamentals and Practical Methods” (written and edited by Mitsuo Tasumi, Spectroscopical Society of Japan; S. T. Japan INC. April 2012), “Part II Various Measurement Methods 21. Two-Dimensional Correlation Spectroscopy” (pages 158 to 165) may be referred to. The data illustrated in FIG. 6 is obtained for each frequency used when Che sample s is vibrated with the vibration frequency f[kHz] by the piezoelectric element 43. By virtue of this, the optically active amount can be measured in accordance with the vibration frequency f.


In addition, as illustrated in FIG. 7, the synchronous correlation spectrum (FIG. 7(a)) and the asynchronous correlation spectrum (FIG. 7(b)) are obtained. The individual figures in FIG. 7 describe the spectrum of the optical rotatory dispersion α*(σ) or the circular polarization dichroism elliptieity θ*(σ) on the right side and the upper side of the respective graphs. The respective graphs illustrated in FIG. 7 can be computed by the control means 14 to be displayed.


Referring to FIG. 7(a) illustrating contour lines of the synchronous correlation spectrum, the spectrum is symmetrical to the diagonal line D1. In contrast, referring to FIG. 7(b) illustrating the contour lines of the asynchronous correlation spectrum, it can be seen that the symmetry to the diagonal line D1 is lost. In view of this, it is possible to determine that a certain structural change has occurred with a certain wave number in the particular vibration frequency f. In this manner, it is made possible to provide the basic data for elucidating the structure related, for example, to water molecule of the biological tissue.


As has been discussed in the foregoing, by externally and forcibly imparting vibrations to give the elastic wave, the differences of dynamic perturbative variation among multiple biological tissues can be observed as an amount of change appearing in the optically active amount or optical physical property amount.


According to the present embodiment, the following effects can be obtained.


When the sample S which is a biological tissue is irradiated with the pulsed light, the biological tissue is vibrated by the piezoelectric element 43. By forcibly imparting vibrations to the biological tissue to cause the biological tissue to vibrate, it is made possible to perform spectroscopic measurement in accordance with the vibration frequency for imparting the vibrations, and obtain an increased amount of information on the biological tissue at the molecule level.


Since the vibration frequency by the piezoelectric element 43 is swept within a predetermined range, it is made possible to identify the structure of a biological molecule in accordance with various frequencies.


When the relaxation time T of the biological tissue is to be obtained as the dynamic physical property, the vibration frequency dependence of the relaxation time T can be revealed, which contributes to the elucidation of the structure of the biological tissue.


REFERENCE SIGNS LIST


1 pulsed laser light source



2 beam splitter (splitting means)



3 terahertz wave generation element (radiation means)



4 detection element (detection means)



5, 6 super-hemispherical silicon lens



7
a first antenna electrode film



7
b second antenna electrode film



8 gap



9 conductive transmission channel



10 discharge electrode



11 first lead



12 second lead



13 modulation means



14 control means



14
a A/D converter



14
b information processing unit



14
c input/output unit



15 holding means



16 optical delay means (for time origin adjustment)



17 optical delay means (for time-series signal measurement)



18 corner cube mirror



19 He—Ne laser



20 driving device (trigger generation circuit)



21, 23 elliptical mirror (aspherical mirror)



22, 24 plane mirror



25 current voltage conversion means



26 lock-in amplifier



27 lens



30 observation unit optical system



41 metamaterial



43 piezoelectric element (vibration device)


S sample (biological tissue)

Claims
  • 1. A method for observing a dynamic physical property of a biological tissue by irradiating the biological tissue with a pulsed light having a wavelength of a far-infrared wavelength region to observe the dynamic physical property of the biological tissue using vibrational optical activity spectroscopy, the method comprising vibrating the biological tissue when the biological tissue is irradiated with the pulsed light.
  • 2. The method for observing the dynamic physical property of the biological tissue according to claim 1, the method comprising: using a radiation means having a photoconductive film receiving a pulse excitation light and generating a photocarrier anda pair of antenna electrode films formed on the photoconductive film and facing each other via a gap, andbeing configured to emit the pulsed light having the wavelength of the far-infrared wavelength region by pulsed laser light irradiation;irradiating the biological tissue with the pulsed light from the radiation means while vibrating the biological tissue; andobserving the dynamic physical property of the biological tissue based on a vibrational circular dichroism spectrum and/or polarization spectroscopy spectrum obtained from a time-series signal of a reflected pulsed light reflected by the biological tissue or a transmitted pulsed light transmitted through the biological tissue.
  • 3. A device for observing a dynamic physical property of a biological tissue, the device comprising a radiation means including a photoconductive film receiving an excitation pulsed laser light and generating a photocarrier andan antenna electrode film formed on the photoconductive film, andconfigured to emit a pulsed light having a wavelength of a far-infrared wavelength region by irradiation of the excitation pulsed laser light;a holding means configured to hold the biological tissue;a vibration device configured to vibrate the holding means;a detection means including a photoconductive film and an antenna electrode film and configured to obtain a time-series signal of a reflected pulsed light reflected by the biological tissue or a transmitted pulsed light transmitted through the biological tissue; anda control means Confiqured to observe the dynamic physical property of the biological tissue based on a vibrational circular dichroism spectrum and/or polarisation spectroscopy spectrum obtained from a signal obtained from the detection means.
Priority Claims (1)
Number Date Country Kind
2016-075572 Apr 2016 JP national
PCT Information
Filing Document Filing Date Country Kind
PCT/JP2017/014149 4/20/2017 WO 00